Gravitation Potential Energy — Question 1

Section 13-5 · Physics pages 1972–1973

Question 1 Equal altitude steps require unequal amounts of lifting work A small mass m is raised quasistatically outside a nonrotating spherical body of mass M and radius R. Use U(r) = −GMm/r, zero at infinity. R 2R 3R Equal radial height increments from R to 2R and from 2R to 3R. (a) Find external work from R to 2R and from 2R to 3R. (b) Compare their sum with the constant-surface-gravity estimate for the same total altitude gain.
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Question 1 - Solution Equal altitude steps require unequal amounts of lifting work R 2R 3R (a) Derivation and calculation Quasistatic motion has ∆K = 0, so external work equals ∆U: Wa→b = U(rb) −U(ra) = GMm ( 1 ra −1 rb ) . Thus W1 = GMm(1/R −1/2R) = GMm 2R , W2 = GMm(1/2R −1/3R) = GMm 6R = W1/3. (b) Result and interpretation The exact total and constant-gravity estimate are Wexact = W1 + W2 = 2GMm 3R , Wgs = mgs(2R) = 2GMm R , Wgs/Wexact = 3 . Gravity weakens during the lift; using its surface value over the entire distance overestimates the required work. Physical check Both segment works are positive, and their sum equals the direct potential change from R to 3R.

Question 1

Equal altitude steps require unequal amounts of lifting work

A small mass mm is raised quasistatically outside a nonrotating spherical body of mass MM and radius RR. Use U(r)=−GMm/rU(r)=-GMm/r, zero at infinity.

Diagram shown in the original SVG worksheet.

  1. Find external work from RR to 2R2R and from 2R2R to 3R3R.

  2. Compare their sum with the constant-surface-gravity estimate for the same total altitude gain.

Question 1 - Solution

Equal altitude steps require unequal amounts of lifting work

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

Quasistatic motion has ΔK=0\Delta K=0, so external work equals ΔU\Delta U: Wa→b=U(rb)−U(ra)=GMm(1ra−1rb).W_{a\to b}=U(r_b)-U(r_a)=GMm\left(\frac1{r_a}-\frac1{r_b}\right). Thus W1=GMm(1/R−1/2R)=GMm2R,\boxed{W_1=GMm(1/R-1/2R)=\frac{GMm}{2R}}, W2=GMm(1/2R−1/3R)=GMm6R=W1/3.\boxed{W_2=GMm(1/2R-1/3R)=\frac{GMm}{6R}}=W_1/3.

(b) Result and interpretation

The exact total and constant-gravity estimate are Wexact=W1+W2=2GMm3R,\boxed{W_{\mathrm{exact}}=W_1+W_2=\frac{2GMm}{3R}}, Wgs=mgs(2R)=2GMmR,Wgs/Wexact=3.W_{g_s}=mg_s(2R)=\frac{2GMm}{R},\qquad \boxed{W_{g_s}/W_{\mathrm{exact}}=3}. Gravity weakens during the lift; using its surface value over the entire distance overestimates the required work.

Physical check

Both segment works are positive, and their sum equals the direct potential change from RR to 3R3R.